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Widening the Axion Window via Kinetic and Stückelberg Mixings
Widening the Axion Window via Kinetic and Stückelberg Mixings

On the Quantum Theory of Line–spectra
On the Quantum Theory of Line–spectra

... In fact we have assumed that the direct transition between two such states cannot be described by ordinary mechanics, while on the other hand we possess no means of defining an energy difference between two states if there exists no possibility for a continuous mechanical connection between them. It ...
Helimagnetic structure of YMn2 observed by means of nuclear
Helimagnetic structure of YMn2 observed by means of nuclear

The AdS/CFT Correspondence arXiv:1501.00007
The AdS/CFT Correspondence arXiv:1501.00007

... as string duality: a strongly coupled limit of any given string theory is equivalent to a weakly coupled limit of another one.7 In other words, as we take the coupling large (i.e. in the gs → ∞ limit), the theory actually simplifies, and can be described perturbatively in some dual variables. Though ...
Mathematics via Symmetry - Philsci
Mathematics via Symmetry - Philsci

... symmetry that relates matter to forces in nature. Supersymmetry requires us to postulate the existence of a partner matter particle for every known particle that carries a force, and a force particle for every matter particle. The idea here is that the laws of physics are invariant if we swap all th ...
Untitled
Untitled

Spin Hamiltonians and Exchange interactions
Spin Hamiltonians and Exchange interactions

... may consider a spin as having a definite direction, just as in the limit of small ~ we may consider an object as having both position and momentum well-defined. Semiclassical spin dynamics This result below can be thought of as the analog for spins of Newton’s equations; the condition for static equ ...
January 20, 2004 9:50 WSPC/140-IJMPB 02353
January 20, 2004 9:50 WSPC/140-IJMPB 02353

Beam Dynamics in High Energy Colliders
Beam Dynamics in High Energy Colliders

Slides - Indico
Slides - Indico

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PERIMETER INSTITUTE L`INSTITUT PERIMETER

... – John Dewey “It doesn’t matter how beautiful your theory is, it doesn’t matter how smart you are. If it doesn’t agree with experiment, it’s wrong.” – Richard P. Feynman ...
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L6 - Physics

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Quantum Gravity as Sum over Spacetimes

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Quantum Mechanics - Nanyang Technological University

The renormalization of the energy-momentum tensor for an effective initial... Hael Collins R. Holman *
The renormalization of the energy-momentum tensor for an effective initial... Hael Collins R. Holman *

Reconstruction of ttZ Events Using Kinematic Likelihood Fits at the
Reconstruction of ttZ Events Using Kinematic Likelihood Fits at the

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Constraint Effective Potential of the Magnetization - Uwe

Finite-Volume Electromagnetic Corrections to the Masses of Mesons
Finite-Volume Electromagnetic Corrections to the Masses of Mesons

... when the electromagnetic gauge field is subject to periodic boundary conditions (PBCs) [15–17]. However, a uniform background charge density can be introduced to circumvent this problem and restore these laws. This is equivalent to removing the zero modes of the photon in a finite-volume (FV) calcul ...
Manifestation and Origin of the Isotope Effect
Manifestation and Origin of the Isotope Effect

Introduction to Loop Quantum Gravity and Spin Foams
Introduction to Loop Quantum Gravity and Spin Foams

A pseudo-mathematical pseudo-review on 4d N = 2
A pseudo-mathematical pseudo-review on 4d N = 2

... The author’s opinion is that we need to push this view point one step further, by regarding QFTs themselves as objects in something like a category. The important point is that a QFT (although not usually rigorously constructed mathematically) is a mathematical object, much like a group, a space or ...
Non-equilibrium and local detection of the normal fraction of a
Non-equilibrium and local detection of the normal fraction of a

Holographic quantum error-correcting code
Holographic quantum error-correcting code

A CP - Indico
A CP - Indico

Tau_Leptons_in_the_Quest_for_New_Physics
Tau_Leptons_in_the_Quest_for_New_Physics

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Quantum chromodynamics

In theoretical physics, quantum chromodynamics (QCD) is the theory of strong interactions, a fundamental force describing the interactions between quarks and gluons which make up hadrons such as the proton, neutron and pion. QCD is a type of quantum field theory called a non-abelian gauge theory with symmetry group SU(3). The QCD analog of electric charge is a property called color. Gluons are the force carrier of the theory, like photons are for the electromagnetic force in quantum electrodynamics. The theory is an important part of the Standard Model of particle physics. A huge body of experimental evidence for QCD has been gathered over the years.QCD enjoys two peculiar properties:Confinement, which means that the force between quarks does not diminish as they are separated. Because of this, when you do separate a quark from other quarks, the energy in the gluon field is enough to create another quark pair; they are thus forever bound into hadrons such as the proton and the neutron or the pion and kaon. Although analytically unproven, confinement is widely believed to be true because it explains the consistent failure of free quark searches, and it is easy to demonstrate in lattice QCD.Asymptotic freedom, which means that in very high-energy reactions, quarks and gluons interact very weakly creating a quark–gluon plasma. This prediction of QCD was first discovered in the early 1970s by David Politzer and by Frank Wilczek and David Gross. For this work they were awarded the 2004 Nobel Prize in Physics.The phase transition temperature between these two properties has been measured by the ALICE experiment to be well above 160 MeV. Below this temperature, confinement is dominant, while above it, asymptotic freedom becomes dominant.
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